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Tilings
Equilateral polygons: Periodic tilings
Pentagon
Tiling: covering the plane without gaps or overlaps
gaps
Aperiodic tiling: no invariance by translation
Penrose Tiling
A negative example to the Hilbert’s 18th problem
R. Penrose (1974)
Aperiodic tiling: no invariance by translation
Penrose Tiling
A negative example to the Hilbert’s 18th problem
R. Penrose (1974)
Building up of space from congruent polyhedra
The Nobel Prize in Chemistry 2011 was awarded to
Shechtman "for the discovery of quasicrystals".
Quasicrystals
D. Shechtman, I. Blech,
D. Gratias, and J. W. Cahn,
PRL, 53, 1951 (1984).
Complete Order:
Periodic Crystals
Quasicrystals
The role of quasicrystals
Complete Disorder:
Non-Crystalline
Complete Order:
Periodic Crystals
What’s More ?
Quasicrystals
The role of quasicrystals
Complete Disorder:
Non-Crystalline
Complete Order:
Periodic Crystals
Quasicrystals
What’s More ?
Quasicrystals
The role of quasicrystals
Complete Disorder:
Non-Crystalline
Complete Order:
Periodic Crystals
Quasicrystals Glass
What’s More ?
Quasicrystals
The role of quasicrystals
Complete Disorder:
Non-Crystalline
Complete Order:
Periodic Crystals
Quasicrystals Glass
What’s More ?
Quasicrystals
The role of quasicrystals
Complete Disorder:
Non-Crystalline
unknown
Yves Meyer
Meyer’s work:
1964-1973 QCs from Harmonic Analysis and Number Theory
1974-1984 Calderón-Zygmund operator theory
1983-1993 Wavelet
1994-1999 Navier-Stokes equation
2000-now QCs and Applications
2010 Gauss Prize
2017 Able Prize
Starting point: the local controls the global
Meyer’s work
Problems :
How to construct
The properties of
Starting point: the local controls the global
Meyer’s work
Problems :
How to construct
The properties of
A trivial case: is a periodic function
Cut-and-Project scheme
A constructive method (Meyer, 1972)
High-D: Periodic Lattice
Window: irrational slice
Low-D: Meyer’s QCs
Cut-and-project scheme can generate tilings.
Dendrimer Liquid QC
The First Soft QCs
X. Zeng, G. Ungar, Y. Liu, V. Percec, A. E. Dulcey, J. K. Hobbs, Nature, 428, 157 (2004).
C12H25
QCs: Discovery
Type of
quasicrystal
d-D n-D Metric Symmetry System First
Report
Icosahedral 3 D 6 5 m 3
_
5_
AlMn Shechtman et al.
1984
Tetrahedral 3D 6 3 m 3
_
AlLiCu Donnadieu, 1994
Decagonal 2D 5 (5) 10/mmm AlMn Chattopadhyay et al.,
1985a and Bendersky,
1985
Dodecagonal 2D 5 3 12/mmm NiCr Ishimasa et al.
1985
Octagonal 2D 5 2 8/mmm VNiSi,
CrNiSi
Wang et al.
1987
Pentagonal 2D 5 (5) 5m_
AlCuFe Bancel , 1993
Natural
Icosahedral
3D 6 (5) m 3
_
5_
khatyrkite Bindi, 2009
Metallic QCs Soft QCs
Soft matter
systems
Type of
quasicrystal
First
Report
Dendrimer liquid
crystals
Dodecagonal Zeng et al.,
2004
ABC star
copolymers
Dodecagonal Hayashida et al.
2007
Colloidal
nanoparticale
Dodecagonal Talapin, 2009
Colloidal coplymer
micelles
nanoparticale
18-fold
Fischer, et al.,
2011
ABA'C tetrablock
terpolymers
Dodecagonal Zhang, Bates,
2012
Mesoporous silica
micelles
Dodecagonal Xiao et al.
2012
Mesoporous silica
nanparticles
Dodecagonal Sun et al. 2017
http://home.iitk.ac.in/~anandh/E-book/Quasicrystals.ppt
2 31
Successive spots are at a distance inflated by
Mg23Zn68Y9 alloy (5-fold)
Experimental QCs
Experimental QCs
∩Meyer’s QCs
4
Quasicrystals : Quasiperiodic Crystals
(Levine-Steinhardt, 1986; Mermin, 1999)
Physical QCs
Diffraction of pattern of
10-fold symmetry in experiment
bj are reciprocal primitive vectors.
b1
b2
b3b4
Numerical Mathematics
Projection method
Crystalline approximant method
One/multi mode approximation
Outline
Finite domains, suitable boundary conditions
Evaluate the energy density to high precision
Put different kinds of ordered structures on an equal footing
Infinite systems without decay
Difficulties in Computing QCs
Diophantine Approximation
Approximate AP function
Diophantine inequality
Continued fraction approximation
Diophantine Approximation
Approximate AP function
Diophantine inequality
Continued fraction approximation
Idea: use a (large) periodic crystal to approximate a QC
Crystalline approximant method (CAM)
Frequency domain: satisfies Diophantine inequality
irrational number
Error : 1. Finity approx. Infinity (Diophantine Approximation error);
2. Numerical error
Error of CAM
Error : 1. Finity approx. Infinity (Diophantine Approximation error);
2. Numerical error (small)
Error of CAM
2D 12 fold symmetric QC
Computational domain:
Error : 1. Finity approx. Infinity (Diophantine Approximation error);
2. Numerical error (small)
Error of CAM
2D 12 fold symmetric QC
Computational domain:
2D 10 fold symmetric QC
Error : 1. Finity approx. Infinity (Diophantine Approximation error);
2. Numerical error (small)
Error of CAM
ESDA 0.1669 0.0918 0.0374 0.0299 …
L 126 204 3372 53654 …
A d-D QC can be embedded into an n-D periodic structure
Implement in Fourier space
Projection Method: Motivation
12-fold symmetry in Fourier domain
Projection matrix:
Projection Matrix
(1, 0, 0, 0)
(0, 1, 0, 0)
(0, 0, 1, 0)
(0, 0, 0, 1)
Frequency set : high-dimension representation
Projection matrix: connects high-D and low-D
Projection method
Periodic crystals: P = Id
Implement in an n-D unit cell
Assume that
Projection Method
In projection method, the energy density can be evaluated by
Theorem: For a d-dimensional quasicrystal , using the
projection method expansion, we have
Projection Method
Presuppose some properties of structures
6-fold symmetry and
Qualitative analysis
Be available to limited cases
One(Multi)-Modes Approximation
Phase Field Crystal Models
Expansion of the free energy with respect to
Periodic crystals: one length scale
QCs: two length scales
Comparison
Take Lifshitz-Petrich model (PRL, 1997 ) as an example
Projection method can obtain exact energy density.
Comparison
Take Lifshitz-Petrich model (PRL, 1997 ) as an example
Projection method can obtain exact energy density.
Comparison
Take Lifshitz-Petrich model (PRL, 1997 ) as an example
Projection method can obtain exact energy density.
Comparison
Take Lifshitz-Petrich model (PRL, 1997 ) as an example
Projection method can obtain exact energy density.
Projection Method
Comparison
Take Lifshitz-Petrich model (PRL, 1997 ) as an example
Projection method can obtain exact energy density.
Comparison
Take Lifshitz-Petrich model (PRL, 1997 ) as an example
Projection method can obtain exact energy density.
No Diophantine Approximation
Projection method (PM) costs less CPU time.
Comparison
Modes PM CAM (L=30)
4 -3.469032257481E-03 -3.4712487912555E-03
6 -3.527308744797E-03 -3.4832422187171E-03
8 -3.524067379524E-03 -3.4578379603209E-03
16 -3.524067379522E-03 -3.4578375604919E-03
24 -3.524067379522E-03 -3.4578375604919E-03
32 -3.524067379522E-03 -3.4578375604919E-03
40 -3.524067379522E-03 -3.4578375604919E-03
Projection method (PM) costs less CPU time.
Comparison
Modes PM CAM (L=30)
4 -3.469032257481E-03 -3.4712487912555E-03
6 -3.527308744797E-03 -3.4832422187171E-03
8 -3.524067379524E-03 -3.4578379603209E-03
16 -3.524067379522E-03 -3.4578375604919E-03
24 -3.524067379522E-03 -3.4578375604919E-03
32 -3.524067379522E-03 -3.4578375604919E-03
40 -3.524067379522E-03 -3.4578375604919E-03
The precision is enough.
Figure: Real space densities and their spectra of (a) 12-fold, (b) 10-fold,
(c) 8-fold QCs computed by the Projection Method in the 4-D space .
QCs in LP Model
Projection method can discover more QCs
Diffraction pattern of 3d icosahedral
QCs obtained by projection method
in the 6-D space .
3D Icosahedral QCs
Diffraction pattern of 3d icosahedral
QCs obtained by projection method
in the 6-D space .
3D Icosahedral QCs
Cu-Ga-Mg-Sc alloys ,
Phil. Mag. Lett. 2002, 82, 483
Compare with experiment
Diffraction pattern of 3d icosahedral
QCs obtained by projection method
in the 6-D space .
3D Icosahedral QCs
Cu-Ga-Mg-Sc alloys ,
Phil. Mag. Lett. 2002, 82, 483
Compare with experiment
Two-modes approximation method Projection method
Algorithm plays an important role in studying QCs!
Phase Diagrams
Big
Difference !
What’s a QC in mathematical language ?
Projection method, Cut-and-Projection scheme
Mathematical, Physical, Experimental QCs
Which physical model can produce QCs ?
More structures between perfect crystals and disordered
…
Problems